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SRR-loaded Antipodal Vivaldi Antenna for UWB
Applications with Tunable Notch FunctionDebdeep Sarkar
#1, Kumar Vaibhav Srivastava
#2,Member, IEEE
#Department of Electrical Engineering, Indian Institute of Technology, Kanpur
1 [email protected]@iitk.ac.in
Abstract This paper presents design of a novel compact
UWB antipodal Vivaldi antenna, where band-notch
characteristics within 5-6 GHz frequency range is achieved by
placing a parasitic rectangular SRR near the radiating arm, in
order to reduce electromagnetic interference with IEEE 802.11a
and HIPERLAN/2 systems. Simulation results show that the
proposed antenna provides wide impedance band-width with
satisfactory rejection in the desired band along with good gain
and stable radiation pattern in the rest of the UWB regime.
I.
INTRODUCTIONDesign of Ultra-Wideband (UWB) antennas for
state-of-the-art wireless communication has drawn
the attention of researchers since FCC first
approved the rules for the commercial utilization of
the unlicensed 3.1-10.6 GHz frequency band [1].
Various UWB antenna topologies have been
proposed in order to overcome the challenges of
achieving good impedance matching and radiation
stability within compact size and low
manufacturing cost [2-3]. Among them, antipodal
Vivaldi antennas (AVA) are attractive choice due totheir broad impedance bandwidth, symmetric end-
fire beam and ease of implementation in planar
PCB technology [4-6].
Electromagnetic Interference (EMI) due to the
existing narrowband communication systems like
WiMAX, WLAN (IEEE 802.11a, HIPERLAN-2)
and X-band systems is one of the major concerns
for UWB antenna engineers. Instead of using
additional band-stop filters (which would increase
antenna-footprint) for providing the desired notch-
band, the approach of embedding different-shaped
slots (C-shaped, H-shaped) in the radiator or ground
plane of the antenna, acting as intrinsic filters, have
become very popular in the antenna community [7-
8]. Meta-resonators like complementary split-ringresonators (CSRRs) have also found application in
design of UWB antennas with multiple notch-bands
[9].
This paper proposes a novel compact AVA
where the notch-band in the 5-6 GHz band is
achieved by properly placing a single rectangular
split-ring resonator (SRR) in vicinity of the
radiating arm of the antenna. The SRR acts as a
sub-wavelength resonator (size: /10-by-/12 with
respect to the notch frequency) and produces the
desired band-rejection in the IEEE 802.11a and
HIPERLAN/2 WLAN frequencies along with stable
far-field radiation pattern in the radiating band.
The paper is organised as follows. In section-II,
design of the reference AVA is presented. In
section-III, the comparison of the proposed and
reference AVA are shown, which is followed by
concluding discussions in section-IV.
II. DESIGN OF REFERENCE UWB AVA
The geometry of the reference balanced antipodal
Vivaldi antenna is shown in Fig.1. The tapered
radiation structure is designed from the intersection
of two quarter-ellipses according to the principle
followed in [5].
Fig. 1. Geometry of the balanced antipodal Vivaldi antenna which usesdesign principle in [5] (unit: mm)
Copyright 2013 IEICE
Proceedings of the "2013 International Symposium on Electromagnetic Theory"
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Metallization is provided symmetrically on both
sides of the 1.6 mm thick FR-4 epoxy substrate
(dielectric constant = 4.4, loss tangent tan = 0.02)
as is evident from Fig. 1. FEM-based commercial
electromagnetic simulator HFSS is used for
simulation of the antenna. It is found fromsimulation-results that the antenna provides good
impedance bandwidth matching (VSWR < 2) over
the UWB frequency range (3.1-10.6 GHz) along
with good far-field gain.
III.DESIGN OF SINGLE BAND-NOTCHED UWB AVA:RESULTSAND COMPARISON
A.Dimensions and Positioning of Parasitic Split-Ring
Resonator
The frequency response of a rectangular split ring
resonator (SRR) placed in microstriplineenvironment is studied by principle adopted in [10]
for different structural parameters (length and width
of split-rings, ring-spacing, split-gap dimensions).
To provide the desired notch-band, the rectangular
SRR is placed near one radiating arm of the
reference AVA as a parasitic element. The
dimensions of the SRR (as shown in Fig. 2) are
chosen such that its fundamental resonance
frequency lies in the middle of WLAN frequency
band (5.15-5.85 GHz).
Next the SRR position is varied to find outwhere the best band-notch characteristics in the
desired frequency range is achieved without
disturbing the impedance matching in other
frequency bands. Fig. 3 shows VSWR plots of the
antenna for the positions of the SRR with respect to
the AVA. It is observed that for position-1, the band
rejection is not at all satisfactory. For position-3,
although we get band-rejection in desired WLAN
range, impedance-matching deteriorates for higher
frequency. Hence for the proposed SRR-loaded
AVA, position-2 is chosen as optimum (Fig. 4).
Fig. 2. Dimensions of the rectangular SRR used as parasitic element (unit:
mm)
Fig. 3. Plot of VSWR of the band-notched antenna with respect to the
frequency for three different positions of the SRR
B.Performance of single SRR-loaded AVA
The variation of VSWR with frequency for the
proposed AVA as well as the reference antenna as
shown in Fig. 1 is illustrated in Fig. 5. It is observed
that the proposed antenna has impedance band-
width (3.1-11.4 GHz) covering the entire UWBspectrum along with the notch band in the
frequency range (5.15-6.07 GHz) which
encompasses the upper-WiMAX/WLAN band. The
maximum band-notch is achieved at 5.55 GHz
(VSWR=6.399).
Fig. 6 shows the comparison of peak realized far-
field gain of the proposed and reference antenna in
the range 3-11 GHz. It is seen that the gain-plot of
the proposed antenna closely follows that of the
reference UWB antenna, except the desired notch
band where a strong dip is observed.
Fig. 4. Proposed band-notched AVA with optimized SRR dimension and
position (unit: mm)
Fig. 5. VSWR versus frequency plots of the proposed antenna and the
reference antenna
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Fig. 7 shows the vector-plot of the surface
current distribution on the radiating arms of the
antenna as well as the SRR at three frequencies, the
middle one being the notch frequency at 5.55 GHz
to give an insight into the radiation-mechanism and
the band-rejection principle of the proposed AVA.
Strong surface-current density on the SRR, whichacts as a high Q-resonator at the notch frequency
5.55 GHz, compared to that on the radiating arms
suggest the reason for non-radiating behaviour of
the proposed AVA in the desired notch band.
Fig. 6. Peak-gain (dBi) versus frequency plots of the proposed antenna and
the reference antenna
Fig. 8 and Fig. 9 respectively show the 3D-gainplots of the reference and proposed band-notched
AVA at 4 GHz (below the notch frequency) and 8
GHz (above the notch frequency). It is evident that
the far-field radiation pattern is not seriouslyaffected due to the presence of the parasitic SRR.
C.Performance of identical antenna-pairs in far-field
To validate that the proposed antenna
successfully blocks out the desired notch band, we
perform the simulation of a transceiver antenna
system, keeping the two identical antennas in far-field (distance between antennas = 90 mm). Fig. 10
shows the simulated magnitude (dB) and phase (in
degrees) of the S21for the two-antenna system. The
magnitude of the transmission coefficient S21 (dB)
shows a dip in the desired region. The variation of
phase of S21 with frequency also implies the
presence of notch-band.
Fig. 7. Surface Current Distributions on the antenna conductors and SRR
at three different frequencies
Fig. 8. 3D-gain plots of the reference AVA at 4 GHz (top) and 8 GHz
(bottom) respectively
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Fig. 8. 3D-gain plots of the proposed AVA at 4 GHz (top) and 8 GHz (bottom)respectively
Fig. 10. Magnitude (dB) and phase (in degree) of S21for two identical band-
notched AVA placed in far-field region
IV.CONCLUSION
An SRR-loaded antipodal Vivaldi antenna having
UWB characteristics with notch band in the 5-6
GHz frequency range has been designed. The
impedance bandwidth and far-field behavior of the
proposed antenna has been investigated by HFSS
simulations.The proposed antenna is low-profile and uses
low-cost FR-4 substrate. To validate the simulation
results, the antenna would be fabricated and tested
in near future. Since the band-rejection property is
achieved via the rectangular SRR element placed
near the radiating arm of the antenna, it can be
tuned by changing SRR dimensions and positions.
Hence, multiple band-notched antennas for UWB
applications can be designed using the principle
used in this paper.
ACKNOWLEDGMENT
The authors would like to acknowledge all the
members of the Microwave circuit and Microwave
Metamaterials Laboratory (Department of Electrical
Engineering, IIT Kanpur) for their inspiration and
IIT Kanpur authority for the financial assistance.
REFERENCES
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[3] Y. J. Ren and K. Chang, An Annular Ring Antenna for UWBCommunications, vol. 5, no. 1, pp. 274-276, 2006.
[4] E. Gazit, Improved design of the Vivaldi antenna, IEE Proceedings
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[7] X. L. Bao and M. J. Ammann, Printed band-reject UWB antenna with
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[9] J. Kim, C. S. Cho, and J. W. Lee, 5.2 GHz notched ultra-wideband
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